Write u=1/T. Then logζ=constant−(3/4)logu−THu, giving local slope dlog10ζ/du=−(TH+3T/4)/log10. At 5000–6000 K its magnitude is about 3.6×104 K. The low-ionization tail in the original graph drops roughly one decade per 2.8×10−5 K−1, consistent with this value.
At u=2.0×10−4 K−1, the graph gives T≃5000 K and ζ≃0.004. Invert the full equation to get n=CT3/2e−R/(kBT)(1−ζ)/ζ2, yielding n∼1018 m−3. The neighboring tail markers give the same order; plotting precision and the squared dependence on the read ionization fraction preclude claiming many significant digits.
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